Legendre rational functions

In mathematics the Legendre rational functions are a sequence of functions which are both rational and orthogonal. A rational Legendre function of degree n is defined as:

$R_{n}(x)\equiv {\frac {\sqrt {2}}{x+1}}\,L_{n}\left({\frac {x-1}{x+1}}\right)$

where $L_{n}(x)$ is a Legendre polynomial. These functions are eigenfunctions of the singular Sturm-Liouville problem:

$(x+1)\partial _{x}(x\partial _{x}((x+1)v(x)))+\lambda v(x)=0$

with eigenvalues

$\lambda _{n}=n(n+1))\,$.

Properties

Many properties can be derived from the properties of the Legendre polynomials of the first kind. Other properties are unique to the functions themselves.

Recursion

$R_{n+1}(x)={\frac {2n+1}{n+1}}\,{\frac {x-1}{x+1}}\,R_{n}(x)-{\frac {n}{n+1}}\,R_{n-1}(x)\quad \mathrm {for\,n\geq 1}$

and

$2(2n+1)R_{n}(x)=(x+1)^{2}(\partial _{x}R_{n+1}(x)-\partial _{x}R_{n-1}(x))+(x+1)(R_{n+1}(x)-R_{n-1}(x))$

Limiting behavior

It can be shown that

$\lim _{x\rightarrow \infty }(x+1)R_{n}(x)={\sqrt {2}}$

and

$\lim _{x\rightarrow \infty }x\partial _{x}((x+1)R_{n}(x))=0$

Orthogonality

$\int _{0}^{\infty }R_{m}(x)\,R_{n}(x)\,dx={\frac {2}{2n+1}}\delta _{nm}$

where $\delta _{nm}$ is the Kronecker delta function.

Particular values

$R_{0}(x)=1\,$

$R_{1}(x)={\frac {x-1}{x+1}}\,$

$R_{2}(x)={\frac {x^{2}-4x+1}{(x+1)^{2}}}\,$

$R_{3}(x)={\frac {x^{3}-9x^{2}+9x-1}{(x+1)^{3}}}\,$

$R_{4}(x)={\frac {x^{4}-16x^{3}+36x^{2}-16x+1}{(x+1)^{4}}}\,$

References

Zhong-Qing, Wang (2005). "A mixed spectral method for incompressible viscous fluid flow in an infinite strip" (PDF). Mat. apl. comput. 24 (3). doi:10.1590/S0101-82052005000300002. Retrieved 2006-08-08. {{cite journal}}: Cite has empty unknown parameter: |month= (help); Unknown parameter |coauthors= ignored (|author= suggested) (help)